US20240183075A1 - METHOD OF PRODUCING LARGE EMI SHIELDED GaAs AND GaP INFRARED WINDOWS - Google Patents
METHOD OF PRODUCING LARGE EMI SHIELDED GaAs AND GaP INFRARED WINDOWS Download PDFInfo
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- 229910001218 Gallium arsenide Inorganic materials 0.000 title claims abstract description 57
- 238000000034 method Methods 0.000 title claims description 36
- 238000001771 vacuum deposition Methods 0.000 claims abstract description 8
- 238000004519 manufacturing process Methods 0.000 claims abstract description 7
- 238000005498 polishing Methods 0.000 claims description 17
- 239000006117 anti-reflective coating Substances 0.000 claims description 5
- 239000013078 crystal Substances 0.000 abstract description 6
- 238000000576 coating method Methods 0.000 abstract description 5
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 46
- 229910000154 gallium phosphate Inorganic materials 0.000 description 39
- LWFNJDOYCSNXDO-UHFFFAOYSA-K gallium;phosphate Chemical compound [Ga+3].[O-]P([O-])([O-])=O LWFNJDOYCSNXDO-UHFFFAOYSA-K 0.000 description 39
- 239000005083 Zinc sulfide Substances 0.000 description 11
- 229910052984 zinc sulfide Inorganic materials 0.000 description 11
- 230000003287 optical effect Effects 0.000 description 10
- 239000002243 precursor Substances 0.000 description 7
- 239000000463 material Substances 0.000 description 6
- 235000012431 wafers Nutrition 0.000 description 4
- 239000004065 semiconductor Substances 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 238000000927 vapour-phase epitaxy Methods 0.000 description 3
- 239000011248 coating agent Substances 0.000 description 2
- 238000005520 cutting process Methods 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 2
- 238000000151 deposition Methods 0.000 description 2
- 230000008021 deposition Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 238000002488 metal-organic chemical vapour deposition Methods 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000001451 molecular beam epitaxy Methods 0.000 description 2
- 230000003595 spectral effect Effects 0.000 description 2
- 229910005540 GaP Inorganic materials 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 239000002019 doping agent Substances 0.000 description 1
- 239000012467 final product Substances 0.000 description 1
- HZXMRANICFIONG-UHFFFAOYSA-N gallium phosphide Chemical compound [Ga]#P HZXMRANICFIONG-UHFFFAOYSA-N 0.000 description 1
- 125000002524 organometallic group Chemical group 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- DRDVZXDWVBGGMH-UHFFFAOYSA-N zinc;sulfide Chemical compound [S-2].[Zn+2] DRDVZXDWVBGGMH-UHFFFAOYSA-N 0.000 description 1
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- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
- C30B29/10—Inorganic compounds or compositions
- C30B29/40—AIIIBV compounds wherein A is B, Al, Ga, In or Tl and B is N, P, As, Sb or Bi
- C30B29/42—Gallium arsenide
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/22—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the deposition of inorganic material, other than metallic material
- C23C16/30—Deposition of compounds, mixtures or solid solutions, e.g. borides, carbides, nitrides
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/22—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the deposition of inorganic material, other than metallic material
- C23C16/30—Deposition of compounds, mixtures or solid solutions, e.g. borides, carbides, nitrides
- C23C16/301—AIII BV compounds, where A is Al, Ga, In or Tl and B is N, P, As, Sb or Bi
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
- C30B29/10—Inorganic compounds or compositions
- C30B29/40—AIIIBV compounds wherein A is B, Al, Ga, In or Tl and B is N, P, As, Sb or Bi
- C30B29/44—Gallium phosphide
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B33/00—After-treatment of single crystals or homogeneous polycrystalline material with defined structure
- C30B33/06—Joining of crystals
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T428/00—Stock material or miscellaneous articles
- Y10T428/16—Two dimensionally sectional layer
- Y10T428/162—Transparent or translucent layer or section
Definitions
- the disclosure relates to optical windows, and more particularly, to GaAs optical windows that are more than eight inches in diameter and GaP optical windows that are more than four inches in diameter.
- IR infrared
- lasers that operate over a wide range of wavelengths between one and twelve microns. Accordingly, the platforms on which these devices are mounted require optical windows that are transparent over this broad spectral range.
- a growing number of these applications require windows having a largest diameter of more than 8 inches, and in some cases more than 12 inches, which in turn requires that the window material must be relatively hard, so that the window will be structurally competent without being unduly thick.
- EMI electromagnetic shielding
- HIP hot-isostatic-pressed
- ZnS polycrystalline Zinc Sulfide
- the mechanical properties of HIP ZnS are only adequate at best, which can sometimes limit application of the material to large IR windows, such as IR windows greater than 12 inches in diameter.
- HIP ZnS is generally produced by first growing crystalline ZnS by CVD, and then applying the additional step of HIP, which of course adds to the cost of the final product.
- HIP ZnS windows When EMI shielding is required, HIP ZnS windows generally rely on a metallic grid coating deposited onto a window surface.
- the metal lines in the grid coating are opaque to IR radiation, obscuring portions of the window, and can significantly reduce the optical transmission of the window, especially at large angles of incidence. Additionally, the grid pattern can lead to diffraction of IR waves passing through the material, which can have substantial negative impacts on system performance.
- IR windows made from gallium arsenide (GaAs) or gallium phosphate (GaP) are a potential alternative to windows made from HIP ZnS.
- GaAs is highly transparent from 1.7 to 12 microns, exhibits about 3.5 ⁇ higher hardness compared to HIP ZnS, and can be easily and precisely doped to control the electrical properties of thin epitaxially applied conducting layers.
- Gallium phosphide, GaP is highly transparent between 0.7 and 8.5 microns, and does not absorb strongly until nearly 11 microns. It has an even higher mechanical strength than GaAs, and substantially higher visible and near-IR transparency than GaAs, at the expense of reduced transparency at longer wavelengths. Like GaAs, GaP can also be easily and precisely doped to control the electrical properties of thin, epitaxially applied conducting layers.
- GaAs and GaP substrate wafers are cut from single crystals grown by melt techniques, primarily Czochralski (Cz) or Vertical Gradient Freeze (VGF) growth.
- IC's, solar cells, and other multi-layer device structures are typically then grown on these substrates by epitaxial methods such as Molecular Beam Epitaxy (MBE) or Metal Organic Vapor Phase Epitaxy (MOVPE) with precisely controlled layer thicknesses.
- MBE Molecular Beam Epitaxy
- MOVPE Metal Organic Vapor Phase Epitaxy
- GaAs and GaP as slab materials for large IR windows, e.g. for GaP windows having a largest dimension that is greater than 4 inches, and for GaAs windows having a largest dimension that is greater than 8 inches, and up to 12 inches and more.
- the present disclosure is a method of making GaAs slabs having largest dimensions that are greater than 4 inches, and GaP slabs having largest dimensions that are greater than 8 inches, and preferably equal to 12 inches or more, wherein the slabs are sufficiently thick to be structurally competent when used as IR windows. It will be understood that the present disclosure is not limited to producing slabs shaped as disks, and that references herein to the “diameter” of a slab refer to a size of the largest dimension of the slab, unless otherwise required by context.
- the present disclosure teaches slicing slabs of smaller diameter from GaAs or GaP single crystal boules, such as 6-inch GaAs boules, 8-inch GaAs boules, or 3-inch GaP boules, and then “dicing” the slabs to form even smaller rectangular parallelepiped slabs, referred to herein simply as “rectangular” slabs.
- the rectangular slabs are then ground, such that they have precisely perpendicular edges, and then transformed into “precursor” slabs by polishing the surrounding sides of the rectangular slabs to be ultra-flat and ultra-smooth.
- the surrounding sides of the rectangular slabs will be relatively smaller in area, and will surround the largest surfaces of the rectangular slabs.
- the polished surrounding sides of the precursor slabs have a flatness of at least ⁇ /10, and a roughness Ra of less than 10 nanometers.
- the rectangular slabs are beveled and stacked while being ground, after which the stack is mounted on a precision jig for polishing to form a stack of the precursor slabs.
- the precursor slabs are then aligned and fused edge-to-edge via optical-contacting/bonding techniques to create a large GaAs or GaP window having negligible bond interface losses. Finally, in embodiments the faces of the resulting GaAs or GaP window are ground to remove bevels, and polished.
- EMI shielded GaAs or GaP windows are produced by applying a conductive, doped GaAs or GaP layer to the window, for example in a subsequent vacuum deposition step, for example using an epitaxial method such as molecular beam epitaxy (MBE), metal-organic vapor phase epitaxy (MOVPE), metallo-organic chemical vapor deposition (MOCVD, or organo-metallic vapor phase epitaxy (OMVPE).
- MBE molecular beam epitaxy
- MOVPE metal-organic vapor phase epitaxy
- MOCVD metallo-organic chemical vapor deposition
- OMVPE organo-metallic vapor phase epitaxy
- a first general aspect of the present disclosure is an infrared window comprising a GaP slab having a slab largest dimension that is greater than four inches or a GaAs slab having a slab largest dimension that is greater than eight inches.
- the slab is formed by grinding and polishing surrounding sides of a plurality of rectangular parallelepiped slabs, referred to herein as rectangular slabs, and then aligning and contacting the surrounding sides of the rectangular slabs so as to optically bond the rectangular slabs to each other, thereby forming a monolithic GaP window slab having a largest dimension that is greater than four inches, or a monolithic GaAs window slab having a largest dimension that is greater than eight inches.
- the monolithic window slab has a largest dimension that is greater than 12 inches.
- the surrounding sides of each of the rectangular slabs can surround largest faces of the rectangular slabs.
- all of the rectangular slabs can have a common size and shape.
- Any of the above embodiments can further include a conductive layer of doped GaAs or GaP applied to at least one face of the monolithic window slab.
- Any of the above embodiments can further include an anti-reflective coating applied to at least one face of the monolithic slab.
- a second general aspect of the present disclosure is a method of making a GaAs slab having a largest dimension that is greater than eight inches or a GaP slab having a largest dimension that is greater than four inches, the slab being suitable for forming a GaP infrared (IR) transparent window having a largest dimension that is greater than four inches, or a GaAs infrared (IR) transparent window having a largest dimension that is greater than eight inches.
- IR infrared
- IR GaAs infrared
- the method includes obtaining a boule of GaAs or GaP, slicing the boule to form a plurality of rectangular parallelepiped slabs, referred to herein as rectangular slabs, grinding the rectangular slabs to have precisely perpendicular edges, polishing surrounding sides of each of the rectangular slabs to a high degree of flatness and smoothness, and aligning the surrounding sides of the rectangular slabs with each other and contacting the surrounding sides together so as to optically bond the rectangular slabs to each other, thereby forming a monolithic window slab.
- obtaining the boule includes obtaining the boule from a commercial source.
- polishing surrounding sides of each of the rectangular slabs to a high degree of flatness and smoothness can include polishing the surrounding sides to a flatness of better than ⁇ /10 and to a smoothness with Ra less than 10 nanometers.
- Any of the above embodiments can further include grinding faces of the monolithic window slab to remove bevels.
- Any of the above embodiments can further include polishing faces of the monolithic window slab.
- the monolithic window slab can have a largest dimension that is greater than 12 inches.
- the surrounding sides of each of the rectangular slabs can surround largest faces of the rectangular slabs.
- all of the rectangular slabs can have a common size and shape.
- grinding the rectangular slabs to have precisely perpendicular edges includes arranging the rectangular slabs in a stacked configuration, and grinding sides of the stack.
- polishing surrounding sides of each of the rectangular slabs to a high degree of flatness and smoothness can include arranging the rectangular slabs in a stacked configuration, and polishing sides of the stack. And in some of these embodiments the sides of the stack are polished while the stack is mounted on a precision jig.
- any of the above embodiments can further include applying a conductive layer of doped GaAs or GaP to at least one face of the monolithic window slab.
- the conductive layer is applied using a vacuum deposition process.
- any of the above embodiments can include applying an anti-reflective coating to at least one face of the monolithic slab.
- FIG. 1 A is a perspective view of a boule of GaAs or GaP showing the planes along which it is sliced and cut into rectangular tiles;
- FIG. 1 B is a perspective view of the stack of tiles that result from the slicing and cutting of FIG. 1 A ;
- FIG. 1 C illustrates the stack of tiles of FIG. 1 B being ground to have precisely flat and perpendicular edges
- FIG. 1 D illustrates the sides of the stack of tiles of FIG. 1 C being polished to nanometer-scale roughness while maintaining a high degree of flatness
- FIG. 1 E illustrates the alignment and optical bonding together of a plurality of tiles to form a monolithic slab
- FIG. 1 F illustrates the faces of the monolithic slab of FIG. 1 E being ground to remove bevels and polished;
- FIG. 1 G illustrates application of a conductive semiconductor layer to the monolithic slab of FIG. 1 F by vacuum deposition
- FIG. 2 is a flow diagram illustrating a method embodiment of the present disclosure.
- the present disclosure is a method of making GaAs slabs having largest dimensions that are greater than 4 inches, and GaP slabs having largest dimensions that are greater than 8 inches, and preferably equal to 12 inches or more, wherein the slabs are sufficiently thick to be structurally competent when used as IR windows.
- the present disclosure teaches cutting slices 102 from GaAs or GaP single crystal boules 100 that are less than 12 inches in diameter, such as 6-inch GaAs boules, 8-Inch GaAs boules, or 3-inch GaP boules.
- the method includes obtaining the boules by purchasing them commercially.
- the slices 102 are then “diced” to form smaller rectangular parallelepiped slabs 104 , referred to herein simply as “rectangular” slabs 104 .
- the rectangular slabs 104 are then beveled, stacked, and ground 108 such that they have precisely perpendicular edges.
- the stack is then mounted on a precision jig 106 and transformed into “precursor” slabs 110 by polishing 112 the surrounding, smaller sides of the rectangular slabs 104 to be ultra-flat and ultra-smooth.
- the sides of the precursor slabs 110 have a flatness of at least ⁇ /10, and a roughness Ra of less than 10 nanometers.
- the smaller, surrounding sides of the precursor slabs 110 are then fused edge-to-edge via optical-contacting/bonding techniques to create a large GaAs or GaP window 114 having negligible bond interface losses.
- the faces 116 of the resulting GaAs or GaP window 114 are ground 118 to remove bevels, and polished.
- EMI shielded GaAs or GaP windows 116 are produced by subsequently applying a conductive, doped GaAs or GaP layer to the window 116 , for example by placing the window 116 in a vacuum deposition apparatus 120 and applying the conductive layer by MOCVD, or by another vacuum deposition method, followed, in embodiments, by deposition of electrical contacts and/or single or double-side anti-reflection (AR) coatings.
- a conductive, doped GaAs or GaP layer for example by placing the window 116 in a vacuum deposition apparatus 120 and applying the conductive layer by MOCVD, or by another vacuum deposition method, followed, in embodiments, by deposition of electrical contacts and/or single or double-side anti-reflection (AR) coatings.
- AR anti-reflection
- FIG. 2 is a flow diagram that illustrates an embodiment of the presently disclosed method in which EMI shielded IR windows are produced.
- the method begins by obtaining 200 a commercially produced boule 100 of GaAs or GaP, which is then sliced and diced 202 to form a plurality of rectangular slabs 104 .
- the rectangular slabs are then ground 204 so that they have ultra-perpendicular edges, and the smaller sides of the slabs 104 that surround the largest sides are polished 206 so that they are ultra-flat and ultra-smooth.
- the rectangular slabs 104 are aligned and their smaller edges are brought together such that they are fused 208 by optical bonding to form a single, large window 116 .
- the faces of the window 116 are then ground to remove bevels, and polished 210 .
- a conductive layer of GaAs or GaP is applied 212 to at least one of the faces of the window 116 , for example by vacuum deposition, after which anti-reflective coatings are applied 214 .
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Abstract
Description
- This application is related to co-pending US application 18,072,931 entitled METHOD OF OPTIMIZING THE EMI SHIELDING AND INFRARED TRANSPARENCY OF GaAs IR WINDOWS with first inventor Jeremy B. Reeves, U.S. application Ser. No. 18/073,177 entitled METHOD OF PRODUCING LARGE GaAs AND GaP INFRARED WINDOWS with first inventor Peter G. Schunemann, filed on Dec. 1, 2022, U.S. application Ser. No. 18/073,228 entitled METHOD OF PRODUCING LARGE GaAs AND GaP INFRARED WINDOWS with first inventor Peter G. Schunemann, filed on Dec. 1, 2022, and U.S. application Ser. No. 18/073,179 entitled METHOD OF PRODUCING LARGE EMI SHIELDED GaAs INFRARED WINDOWS with first inventor Peter G. Schunemann, filed on Dec. 1, 2022, all of which are also by the present Applicant, all of which are herein incorporated by reference in their entirety for all purposes.
- The disclosure relates to optical windows, and more particularly, to GaAs optical windows that are more than eight inches in diameter and GaP optical windows that are more than four inches in diameter.
- A growing number of optical systems incorporate infrared (IR) sensors and/or lasers that operate over a wide range of wavelengths between one and twelve microns. Accordingly, the platforms on which these devices are mounted require optical windows that are transparent over this broad spectral range. A growing number of these applications require windows having a largest diameter of more than 8 inches, and in some cases more than 12 inches, which in turn requires that the window material must be relatively hard, so that the window will be structurally competent without being unduly thick.
- Furthermore, as electronics and sensor systems become more highly and densely integrated, the need has increased for electromagnetic shielding (EMI) of components. For systems that require optical windows, it has therefore become increasingly necessary to provide EMI shielded windows, i.e. windows that have very low absorption at wavelengths of interest, while also shielding the window aperture against electromagnetic penetration.
- The material that is most commonly used to manufacture large IR windows is hot-isostatic-pressed (HIP) polycrystalline Zinc Sulfide (ZnS), due to the broad spectral transparency of ZnS, because the HIP process is relatively quick, and because the window size when using this polycrystalline material is limited only by the size of the high-pressure containment vessel in which the HIP is applied. However, the mechanical properties of HIP ZnS are only adequate at best, which can sometimes limit application of the material to large IR windows, such as IR windows greater than 12 inches in diameter. Furthermore, HIP ZnS is generally produced by first growing crystalline ZnS by CVD, and then applying the additional step of HIP, which of course adds to the cost of the final product.
- When EMI shielding is required, HIP ZnS windows generally rely on a metallic grid coating deposited onto a window surface. However, the metal lines in the grid coating are opaque to IR radiation, obscuring portions of the window, and can significantly reduce the optical transmission of the window, especially at large angles of incidence. Additionally, the grid pattern can lead to diffraction of IR waves passing through the material, which can have substantial negative impacts on system performance.
- In many cases, to provide EMI shielding, it would be preferable to deposit a thin conducting layer of a doped semiconductor onto a surface of an IR window, as an alternative to a metallic grid. Unfortunately, is nearly impossible to dope ZnS to produce a conductive EMI layer, due to its tendency to form compensating defects that neutralize dopants to maintain their insulating properties. This problem can be circumvented by preparing a separate, thin wafer of a doped semiconductor such as GaAs, and then attaching the wafer to the surface of an HIP ZnS window by optical bonding. However, this approach can be time consuming, difficult, and expensive.
- As is discussed in more detail in co-pending application Ser. No. 18/072,931, filed on Dec. 1, 2022, which is also by the present Applicant and is incorporated herein by reference, IR windows made from gallium arsenide (GaAs) or gallium phosphate (GaP) are a potential alternative to windows made from HIP ZnS.
- GaAs is highly transparent from 1.7 to 12 microns, exhibits about 3.5× higher hardness compared to HIP ZnS, and can be easily and precisely doped to control the electrical properties of thin epitaxially applied conducting layers.
- Gallium phosphide, GaP, is highly transparent between 0.7 and 8.5 microns, and does not absorb strongly until nearly 11 microns. It has an even higher mechanical strength than GaAs, and substantially higher visible and near-IR transparency than GaAs, at the expense of reduced transparency at longer wavelengths. Like GaAs, GaP can also be easily and precisely doped to control the electrical properties of thin, epitaxially applied conducting layers.
- Relatively small, thin wafers of GaAs and GaP have been widely used in the integrated circuit (IC) and photovoltaic (i.e. solar cell) industries. GaAs and GaP substrate wafers are cut from single crystals grown by melt techniques, primarily Czochralski (Cz) or Vertical Gradient Freeze (VGF) growth. IC's, solar cells, and other multi-layer device structures are typically then grown on these substrates by epitaxial methods such as Molecular Beam Epitaxy (MBE) or Metal Organic Vapor Phase Epitaxy (MOVPE) with precisely controlled layer thicknesses. The total device structures are limited to thicknesses of several microns, and scaling to thicknesses beyond this is precluded by the very slow growth rates achievable by these epitaxial techniques.
- The Cz and VGF techniques used to produce GaAs and GaP substrates for most IC and photovoltaic applications could also be used to produce IR windows by slicing much thicker slabs (several millimeters) from the single crystal boules grown from melt.
- However, commercially available boules of GaAs that are grown from melt by VGF are generally limited to eight inches in diameter or less, while commercially available Boules of GaP are generally limited to only 3 inches in diameter, and even these are not widely available. Furthermore, scaling the existing GaAs melt-growth techniques to larger diameters would be extremely challenging, for both GaAs and GaP, due to the difficulty of extracting more and more heat while controlling the interface shape and crystal quality during growth from ever increasing melt sizes. Managing the high equilibrium vapor pressure during growth—particularly for GaP—becomes problematic at larger boule diameters.
- This inability to produce larger diameter boules has prevented the use of GaAs and GaP as slab materials for large IR windows, e.g. for GaP windows having a largest dimension that is greater than 4 inches, and for GaAs windows having a largest dimension that is greater than 8 inches, and up to 12 inches and more.
- What is needed, therefore, is a method of making GaAs slabs having largest dimensions that are greater than 4 inches, and GaP slabs having largest dimensions that are greater than 8 inches, and preferably equal to 12 inches or more, wherein the slabs are sufficiently thick to be structurally competent when used as IR windows.
- The present disclosure is a method of making GaAs slabs having largest dimensions that are greater than 4 inches, and GaP slabs having largest dimensions that are greater than 8 inches, and preferably equal to 12 inches or more, wherein the slabs are sufficiently thick to be structurally competent when used as IR windows. It will be understood that the present disclosure is not limited to producing slabs shaped as disks, and that references herein to the “diameter” of a slab refer to a size of the largest dimension of the slab, unless otherwise required by context.
- More specifically the present disclosure teaches slicing slabs of smaller diameter from GaAs or GaP single crystal boules, such as 6-inch GaAs boules, 8-inch GaAs boules, or 3-inch GaP boules, and then “dicing” the slabs to form even smaller rectangular parallelepiped slabs, referred to herein simply as “rectangular” slabs.
- The rectangular slabs are then ground, such that they have precisely perpendicular edges, and then transformed into “precursor” slabs by polishing the surrounding sides of the rectangular slabs to be ultra-flat and ultra-smooth. Typically, the surrounding sides of the rectangular slabs will be relatively smaller in area, and will surround the largest surfaces of the rectangular slabs. In embodiments, the polished surrounding sides of the precursor slabs have a flatness of at least λ/10, and a roughness Ra of less than 10 nanometers. In various embodiments, the rectangular slabs are beveled and stacked while being ground, after which the stack is mounted on a precision jig for polishing to form a stack of the precursor slabs.
- The precursor slabs are then aligned and fused edge-to-edge via optical-contacting/bonding techniques to create a large GaAs or GaP window having negligible bond interface losses. Finally, in embodiments the faces of the resulting GaAs or GaP window are ground to remove bevels, and polished.
- In some embodiments, EMI shielded GaAs or GaP windows are produced by applying a conductive, doped GaAs or GaP layer to the window, for example in a subsequent vacuum deposition step, for example using an epitaxial method such as molecular beam epitaxy (MBE), metal-organic vapor phase epitaxy (MOVPE), metallo-organic chemical vapor deposition (MOCVD, or organo-metallic vapor phase epitaxy (OMVPE). In various embodiments, this is followed by deposition of electrical contacts and/or single or double-side anti-reflection (AR) coatings.
- A first general aspect of the present disclosure is an infrared window comprising a GaP slab having a slab largest dimension that is greater than four inches or a GaAs slab having a slab largest dimension that is greater than eight inches. The slab is formed by grinding and polishing surrounding sides of a plurality of rectangular parallelepiped slabs, referred to herein as rectangular slabs, and then aligning and contacting the surrounding sides of the rectangular slabs so as to optically bond the rectangular slabs to each other, thereby forming a monolithic GaP window slab having a largest dimension that is greater than four inches, or a monolithic GaAs window slab having a largest dimension that is greater than eight inches.
- In embodiments, the monolithic window slab has a largest dimension that is greater than 12 inches.
- In any of the above embodiments, the surrounding sides of each of the rectangular slabs can surround largest faces of the rectangular slabs.
- In any of the above embodiments, all of the rectangular slabs can have a common size and shape.
- Any of the above embodiments can further include a conductive layer of doped GaAs or GaP applied to at least one face of the monolithic window slab.
- Any of the above embodiments can further include an anti-reflective coating applied to at least one face of the monolithic slab.
- A second general aspect of the present disclosure is a method of making a GaAs slab having a largest dimension that is greater than eight inches or a GaP slab having a largest dimension that is greater than four inches, the slab being suitable for forming a GaP infrared (IR) transparent window having a largest dimension that is greater than four inches, or a GaAs infrared (IR) transparent window having a largest dimension that is greater than eight inches. The method includes obtaining a boule of GaAs or GaP, slicing the boule to form a plurality of rectangular parallelepiped slabs, referred to herein as rectangular slabs, grinding the rectangular slabs to have precisely perpendicular edges, polishing surrounding sides of each of the rectangular slabs to a high degree of flatness and smoothness, and aligning the surrounding sides of the rectangular slabs with each other and contacting the surrounding sides together so as to optically bond the rectangular slabs to each other, thereby forming a monolithic window slab.
- In embodiments, obtaining the boule includes obtaining the boule from a commercial source.
- In any of the above embodiments, polishing surrounding sides of each of the rectangular slabs to a high degree of flatness and smoothness can include polishing the surrounding sides to a flatness of better than λ/10 and to a smoothness with Ra less than 10 nanometers.
- Any of the above embodiments can further include grinding faces of the monolithic window slab to remove bevels.
- Any of the above embodiments can further include polishing faces of the monolithic window slab.
- In any of the above embodiments, the monolithic window slab can have a largest dimension that is greater than 12 inches.
- In any of the above embodiments, the surrounding sides of each of the rectangular slabs can surround largest faces of the rectangular slabs.
- In any of the above embodiments, all of the rectangular slabs can have a common size and shape. In some of these embodiments, grinding the rectangular slabs to have precisely perpendicular edges includes arranging the rectangular slabs in a stacked configuration, and grinding sides of the stack. In any of these embodiments, polishing surrounding sides of each of the rectangular slabs to a high degree of flatness and smoothness can include arranging the rectangular slabs in a stacked configuration, and polishing sides of the stack. And in some of these embodiments the sides of the stack are polished while the stack is mounted on a precision jig.
- Any of the above embodiments can further include applying a conductive layer of doped GaAs or GaP to at least one face of the monolithic window slab. In some of these embodiments the conductive layer is applied using a vacuum deposition process.
- And any of the above embodiments can include applying an anti-reflective coating to at least one face of the monolithic slab.
- The features and advantages described herein are not all-inclusive and, in particular, many additional features and advantages will be apparent to one of ordinary skill in the art in view of the drawings, specification, and claims. Moreover, it should be noted that the language used in the specification has been principally selected for readability and instructional purposes, and not to limit the scope of the inventive subject matter.
-
FIG. 1A is a perspective view of a boule of GaAs or GaP showing the planes along which it is sliced and cut into rectangular tiles; -
FIG. 1B is a perspective view of the stack of tiles that result from the slicing and cutting ofFIG. 1A ; -
FIG. 1C illustrates the stack of tiles ofFIG. 1B being ground to have precisely flat and perpendicular edges; -
FIG. 1D illustrates the sides of the stack of tiles ofFIG. 1C being polished to nanometer-scale roughness while maintaining a high degree of flatness; -
FIG. 1E illustrates the alignment and optical bonding together of a plurality of tiles to form a monolithic slab; -
FIG. 1F illustrates the faces of the monolithic slab ofFIG. 1E being ground to remove bevels and polished; -
FIG. 1G illustrates application of a conductive semiconductor layer to the monolithic slab ofFIG. 1F by vacuum deposition; and -
FIG. 2 is a flow diagram illustrating a method embodiment of the present disclosure. - The present disclosure is a method of making GaAs slabs having largest dimensions that are greater than 4 inches, and GaP slabs having largest dimensions that are greater than 8 inches, and preferably equal to 12 inches or more, wherein the slabs are sufficiently thick to be structurally competent when used as IR windows.
- With reference to
FIG. 1A , the present disclosure teaches cuttingslices 102 from GaAs or GaPsingle crystal boules 100 that are less than 12 inches in diameter, such as 6-inch GaAs boules, 8-Inch GaAs boules, or 3-inch GaP boules. In embodiments, the method includes obtaining the boules by purchasing them commercially. - With reference to
FIG. 1B , theslices 102 are then “diced” to form smallerrectangular parallelepiped slabs 104, referred to herein simply as “rectangular”slabs 104. - With reference to
FIG. 1C , in embodiments therectangular slabs 104 are then beveled, stacked, andground 108 such that they have precisely perpendicular edges. With reference toFIG. 1D , the stack is then mounted on aprecision jig 106 and transformed into “precursor”slabs 110 by polishing 112 the surrounding, smaller sides of therectangular slabs 104 to be ultra-flat and ultra-smooth. In embodiments, the sides of theprecursor slabs 110 have a flatness of at least λ/10, and a roughness Ra of less than 10 nanometers. - With reference to
FIG. 1E , the smaller, surrounding sides of theprecursor slabs 110 are then fused edge-to-edge via optical-contacting/bonding techniques to create a large GaAs orGaP window 114 having negligible bond interface losses. Finally, with reference toFIG. 1F , thefaces 116 of the resulting GaAs orGaP window 114 are ground 118 to remove bevels, and polished. - With reference to
FIG. 1G , in some embodiments EMI shielded GaAs orGaP windows 116 are produced by subsequently applying a conductive, doped GaAs or GaP layer to thewindow 116, for example by placing thewindow 116 in avacuum deposition apparatus 120 and applying the conductive layer by MOCVD, or by another vacuum deposition method, followed, in embodiments, by deposition of electrical contacts and/or single or double-side anti-reflection (AR) coatings. -
FIG. 2 is a flow diagram that illustrates an embodiment of the presently disclosed method in which EMI shielded IR windows are produced. The method begins by obtaining 200 a commercially producedboule 100 of GaAs or GaP, which is then sliced and diced 202 to form a plurality ofrectangular slabs 104. The rectangular slabs are then ground 204 so that they have ultra-perpendicular edges, and the smaller sides of theslabs 104 that surround the largest sides are polished 206 so that they are ultra-flat and ultra-smooth. - At this point, the
rectangular slabs 104 are aligned and their smaller edges are brought together such that they are fused 208 by optical bonding to form a single,large window 116. The faces of thewindow 116 are then ground to remove bevels, and polished 210. Finally, a conductive layer of GaAs or GaP is applied 212 to at least one of the faces of thewindow 116, for example by vacuum deposition, after which anti-reflective coatings are applied 214. - The foregoing description of the embodiments of the invention has been presented for the purposes of illustration and description. Each and every page of this submission, and all contents thereon, however characterized, identified, or numbered, is considered a substantive part of this application for all purposes, irrespective of form or placement within the application. This specification is not intended to be exhaustive or to limit the invention to the precise form disclosed. Many modifications and variations are possible in light of this disclosure.
- Although the present application is shown in a limited number of forms, the scope of the invention is not limited to just these forms, but is amenable to various changes and modifications. The disclosure presented herein does not explicitly disclose all possible combinations of features that fall within the scope of the invention. The features disclosed herein for the various embodiments can generally be interchanged and combined into any combinations that are not self-contradictory without departing from the scope of the invention. In particular, the limitations presented in dependent claims below can be combined with their corresponding independent claims in any number and in any order without departing from the scope of this disclosure, unless the dependent claims are logically incompatible with each other.
Claims (20)
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